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Electric field pattern

Figure 4.4 Electric field patterns normal modes (Mie, 1908). Figure 4.4 Electric field patterns normal modes (Mie, 1908).
The frequency dependence of e and e" and their magnitudes control the extent to which a substance is able to couple with the microwave radiation and therefore are fundamental parameters for interpreting the dielectric heating phenomenon. Although tan 8 is a helpful parameter for comparing the heating rates of a series of dielectrics with similar physical and chemical characteristics, for more complex mixtures expressions, which take into account the complexity of the electric field pattern, the heat capacity of the compound and the density, have been proposed. [Pg.11]

Figure 3.4. Development of standing waves TE103 resonant cavity electric field pattern. Reprinted with the permission from [1]. Figure 3.4. Development of standing waves TE103 resonant cavity electric field pattern. Reprinted with the permission from [1].
Fig. 5.4 Electric field patterns in parallel-plate electrode systems (a) un-guarded, (b) guarded. Fig. 5.4 Electric field patterns in parallel-plate electrode systems (a) un-guarded, (b) guarded.
The electro-optic effect leads to the modification of the refractive index of a suitable material when an electric field is applied (Figure 8). The electro-optic effect must be present in a photorefractive material, so that the space charge electric field pattern due the relocated charges will lead to a patterned refractive index in the material this is a hologram. [Pg.3650]

FIG. 5.16 (A) Experimental setup for holographic grating recording (B) schematic representation of electric field patterns on a vertically installed sample. [Pg.161]

There are three basic conductor configurations to consider a single conductor located above a flat plane, two conductors running in parallel with each other, and a conductor running inside a cylindrical screen or shield. Let the following notation be used for the inductances and capacitances that will be referred to later. See Reference 19 for formulae that relate these inductances and capacitances to the physical dimensions of the conductors. Reference 25, chapters 10 and 11 give full details of how to calculate the magnetic and electric field patterns of simple and complex shapes, such as. [Pg.373]

The anodes are made of various materials and the choice is determined by the physical conditions, the electric field pattern, current densities, cost and anode corrosion. Anode current densities vary between 10 amperes per metre squared for silicon iron to more than 1000 amperes per metre squared for platinised and lead alloys. [Pg.467]

Fig. 4a-c a General layout of an ESR spectrometer b Block diagram of an ESR spectrometer and c Magnetic and electric field patterns in a standard ESR cavity (reprinted from reference [15]. Copyright 1992 Broker Instruments, Inc.)... [Pg.302]

Figure 1. (Top) Schematic view of a molecular transition dipole /> at a particular orientation within the electric field pattern E, of a subwavelength aperture. (Bottom) Resulting excitation rate vs. lateral displacement for this particular orientation which is proportional to the square of the component of p along E. Adapted from Ref. 13. Figure 1. (Top) Schematic view of a molecular transition dipole /> at a particular orientation within the electric field pattern E, of a subwavelength aperture. (Bottom) Resulting excitation rate vs. lateral displacement for this particular orientation which is proportional to the square of the component of p along E. Adapted from Ref. 13.
Eigenmode 1 is left-handed circularly polarized and propagates in the + z direction with the speed of c/ v. Eigenmode 2 is also left-handed circularly polarized but propagates in the -z direction with the speed of c/y/f. The instantaneous electric field pattern is of opposite sense to the cholesteric helix which is right-handed. [Pg.80]

The radiation pattern is defined as a mathematical function or a graphical representation of the far field (ie, for r 2D IX, with D being the largest dimension of the antenna) radiation properties of the antenna, as a function of the direction of departure of the electromagnetic (EM) wave. A radiation pattern can represent several quantities, such as gain, directivity, electric field, or radiation vector. Consequently, the terms gain pattern, electric field pattern, or radiation vector pattern are used, respectively. [Pg.602]

Figure 5-8. Upper left-hand side frame Refractive index profile at 514.5 nm of a three-layered Si02-Ti02 planar waveguide. Left-hand side column Calculated squared electric-field patterns of the five TE modes. Right-hand side column BriUouin experimental spectra (open circles), calculated spectra (dotted line), and convolution of the calculated spectra with the instrumental response (solid line). The longitudinal sound velocity used in the fit is vi = 5.9 km/s,for m= 0,1, 2, and 3, and Pl = 5.75 km/sjbr m = 4 (Chiasera, 2003b). Figure 5-8. Upper left-hand side frame Refractive index profile at 514.5 nm of a three-layered Si02-Ti02 planar waveguide. Left-hand side column Calculated squared electric-field patterns of the five TE modes. Right-hand side column BriUouin experimental spectra (open circles), calculated spectra (dotted line), and convolution of the calculated spectra with the instrumental response (solid line). The longitudinal sound velocity used in the fit is vi = 5.9 km/s,for m= 0,1, 2, and 3, and Pl = 5.75 km/sjbr m = 4 (Chiasera, 2003b).
By solving Laplace s equation, the internal and external potentials and electric field patterns of the object studied are determined. [Pg.448]

Only the component of optical polarization for which the instantaneous spatial electric field pattern matches the spiraling cholesteric director is strongly reflected. The other component is transmitted with no significant reflection loss. [Pg.205]

Next we consider the spatial distribution of the electric vector along the z axis at one instant of time, e.g., at t =0. We see from Eqs. [59] and [60] that at 2 = 0 the electric vector points along the x axis, as before. As we move along the positive z axis we find the electric vector rotates first to the positive y direction at 2 = wc 12(a) and then to the negative x direction at 2 = ttc/o), etc. Thus the instantaneous electric field pattern traces out a right-handed spiral (see Fig. 4b). All directions are reversed for left circularly polarized light, which is described by the polarization vector... [Pg.218]

On the micro-level of the brain, there are massively many-body-problems which need a reduction strategy to handle with the complexity. In the case of EEG-pictures, a complex system of electrodes measures local states (electric potentials) of the brain. The whole state of a patient s brain on the micro-level is represented by local time series. In the case of, e.g., petit mal epilepsy, they are characterized by typical cyclic peaks. The microscopic states determine macroscopic electric field patterns during a cyclic period. Mathematically, the macroscopic patterns can be determined by spatial modes and order parameters, i.e., the amplitude of the field waves. In the corresponding phase space, they determine a chaotic attractor characterizing petit mal epilepsy. [Pg.21]

Assembly, Conducting Polymers, Electric Field, Pattern, Transfer. [Pg.1077]


See other pages where Electric field pattern is mentioned: [Pg.33]    [Pg.19]    [Pg.21]    [Pg.97]    [Pg.100]    [Pg.28]    [Pg.32]    [Pg.98]    [Pg.12]    [Pg.448]    [Pg.560]    [Pg.364]    [Pg.33]    [Pg.199]    [Pg.172]    [Pg.448]    [Pg.69]    [Pg.197]    [Pg.249]    [Pg.81]    [Pg.433]    [Pg.33]    [Pg.139]    [Pg.213]    [Pg.215]    [Pg.339]    [Pg.132]   
See also in sourсe #XX -- [ Pg.602 ]




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